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Indus-1, Synchrotron Radiation Source (SRS) facility operating at 450 MeV, is
operational at RRCAT, Indore. It emits radiation in VUV range and is being used
for research in Physics and Chemistry. The SRS complex consists of 20 MeV
injector microtron, 700 MeV booster synchrotron and 450 MeV storage ring. In all
these machines the energy to the accelerating particle i.e. electrons, is
imparted by the RF voltages developed across RF cavities. This article describes
the microwave system for the microtron, and the RF systems for the booster
synchrotron and storage ring INDUS-1. The RF System for the ion clearing
electrodes and Radio Frequency Knock Out (RFKO) systems are also described.
INTRODUCTION
The
role of RF system, in synchrotron radiation source (SRS), is to compensate for
SR losses suffered by circulating electrons through the bending magnets and
insertion devices to keep the beam in equilibrium orbit. The RF system also
provides energy for accelerating the beam from injection energy to final energy.
Booster synchrotron and Indus-1 are relatively small rings with perimeters of
28.449 m and 18.996 m respectively. The operating frequency of both the rings is
chosen as 31.613 MHz mainly to avoid ion trapping problems. The booster
synchrotron is operating at harmonic number of three and storage ring is
operating with harmonic number of two. Owing to same RF frequency, the cavities
in both the rings are similar. The main parameters of both the rings are listed
at Table-1.
The
choice of relatively lower RF frequency dictated the use of heavily capacitively
loaded RF cavities for both the rings. The synchrotron cavity is made out of
Aluminium and that in the storage ring is made out of SS and plated internally
with copper. In synchrotron as well as storage ring, the RF system consists of a
synthesized signal generator followed by a chain of amplifiers, the low level
control circuits for frequency, phase and amplitude control of the RF field
across the cavities. The main power amplifier is built using indigenous BEL make
power tetrode tubes.
Pillbox type of cavity operating at 2856 MHz is employed in the microtron to
accelerate the electrons to 20 MeV energy. The cavity generates nearly 1000 kV
accelerating voltage. 5MW microwave source is developed employing S-Band
klystron tube, to power this cavity.
Table-1: Parameters of booster synchrotron and
INDUS-1 storage ring. Figures in brackets correspond to the operation of the
synchrotron at 700 MeV
|
Parameter
|
Synchrotron |
Storage Ring |
|
|
Energy |
450(700) |
450 |
MeV |
|
Beam current |
30 |
100 |
mA |
|
Circumference |
28.449 |
18.97 |
m |
|
Orbital frequency |
10.5379 |
15.806 |
MHz |
|
Harmonic Number |
3 |
2 |
|
|
RF System frequency |
31.613 |
31.613 |
MHz |
|
Synch. Rad. loss |
2.0(11.8) |
3.63 |
keV/turn |
|
Voltage across cavities |
2-15(30) |
30 |
keV |
|
Momentum compaction |
0.16238 |
0.1457 |
|
|
Energy spread |
2.617 |
3.855 |
(10-4 ) |
|
Synch. Osc. Freq. |
11.325 |
30.59 |
kHz |
RF SYSTEM
The RF system for the storage
ring consists of a synthesized signal generator, the low level RF system, the
high power amplifier along its power supply and the RF cavity. Figure 1 shows
the block diagram of booster and storage ring RF system

Fig.1 Schematic of INDUS-1 and Booster RF systems.
The low level RF
System
Low level RF control system
consists of synthesized signal source,0-360o phase shifter, feed
back loops for amplitude, phase and frequency control, Coaxial RF switch to put
RF on & off and Limiter. Synthesized signal generator giving outputs at 31.613
MHz is developed which will also be used to get synchronized RF drive signal for
Indus-2. Amplitude and phase control feedback loops are incorporated to maintain
the amplitude and phase of the cavity gap voltage within 1% and 1o
respectively for proper operation of the machine. The phase loop compares the phase of the RF signal at the
feed of RF cavity with the reference signal phase. The error signal obtained is
used to drive the variable phase shifter which corrects the phase changes in the
amplifier chain. The electronic fast phase shifter is built using BEL make cascode / differential
amplifiers BMC 3028 A and varacter diodes. To get the phase information at
different operating power level limiter circuits have been used. These are
designed to give constant output of +13dBm at with input ranging from -18 dBm to
+13 dBm
The amplitude control loop
measures the accelerating field in the cavity sampled through small coupling
loop. This sampled signal is compared with a reference (amplitude set) signal.
The correction is made by driving the RF attenuator with the error signal, which
in turn controls drive to solid state amplifier.
The tuning loop together with
amplitude control loop compensates for the beam loading effect and temperature
change. The tuning loop maintains the resonance frequency by comparing the
phases between cavity voltage and cavity input signal from transmission lines
feeding to the cavity. The phase detector gives equivalent error signal
proportional to phase difference between the two signals. Resonance control is
achieved by driving the plunger tuners with the help of stepper motors. Total
dynamic range provided is 40 KHz.
During operation of both the
RF systems manual access is not possible hence both R.F. amplifier systems are
made to operate in local mode and remote mode from control room. All the
parameters like cavity gap voltage, forward and reflected powers at cavity,
tuner position, cavity tuning error etc. are monitored and interlocks are
provided for safe operation of the machine.
The RF Amplifier System
The
operating frequency Booster Synchrotron & Indus1 storage ring is 31.613 MHz.
Similar RF power amplifier scheme is employed for both the machines. The RF
system consists of synthesized source, low level RF control system, 150 watts
solid state driver amplifier, tetrode tube based Power amplifier, 7kV/2A
regulated power supply along with many auxiliary supplies, 15/8 “ coaxial
transmission line with circulator and RF cavities. The storage ring is equipped
with Radio frequency Knock Out (RFKO) amplifier systems & Ion clearing
electrodes RF System operating in the frequency range of 1-10 MHz.

Fig. 2 The RF amplifier
system showing the solid state amplifier, circulator, the power amplifier and
the transmission lines.
The RF system ( Fig.2) is
built using indigenous components. In this system, the low level signal of 10 mW
from frequency synthesizer is amplified to 150 watts by solid-state amplifier.
The basic building block of solid-state amplifier is 80 watts amplifier module
built using RF power transistor type S-100-28. To get good linearity, the solid
state amplifier is designed to operate in class AB mode. The total power of 150
watts is obtained by combining 2 modules of 80 watts using hybrid power
combiners. The low & medium power amplifier modules of 1 W & 10W are built using
BEL make RF transistors 2 N 3866, 2 N 5070. These modules operate in class A
mode. The twisted pair transmission line type transformers (BALUNS) are used to
get wide bandwidth. These transformers are made using soft Ni-Zn ferrite core.
The reflectometer with VSWR protection system is developed and incorporated in
the system to monitor forward and reflected output power of solid-state driver
amplifier. The circulator is incorporated at the output of SSA to protect it
from reflected power from the power amplifier.
The final power
amplifier is built using BEL make ceramic power tetrode tube type 4 CX15000. It
operates in class B grid driven configuration. Impedance matching networks with
pi-configuration are used to match the input and output impedances of tube to
standard 50 ohms. Output matching network uses a high power choke and high
voltage RF vacuum variable capacitors. The complete power amplifier is assembled
in a copper shielded box (fig-3) to have proper RF ground and shielding.

Fig. 3 The power
amplifier tube and the output matching network.
The plate of power amplifier is supplied with a 7
kV/ 2A series regulated power supply(Fig-4). This power supply power employs
water cooled triode tubes type 6000 WC giving better than 0.1% regulation. The
series regulated power supply enables very fast switch off of plate bias of the
tetrode tube. 1 kV / 100mA and –250V/300mA regulated power supplies feeds the
screen grid and control grid of 4 CX 15000 tube. The output power from the power
amplifier is transmitted to the cavity through 15/8“
coaxial line. High power Y-junction circulator is used to protect the expensive
tetrode from reflected power from cavity because of mismatch. Co-axial
directional couplers are developed and incorporated in the line and used for
measuring forward and reflected power to and from the RF cavity.
Fig. 4 The high voltage power supply for the INDUS-1 amplifier system.
The RF cavities
Design
Design parameters of rf cavities are listed in Table
I The RF cavity is designed with the help of
SUPERFISH[1]. The accelerating gap being only 20 mm, the transit time factor is
@1
for v=c electrons at energies ³
5 MeV. The frequency sensitivities of various cavity surfaces as calculated by
SUPERFISH are as follows: cavity radius -0.0112 MHz/mm; cavity length -0.0305
MHz/mm; drift tube outer radius -0.06 MHz/mm; capacitive loading disk back
surface -0.0216 MHz/mm and the accelerating gap 0.635 MHz/mm. Unlike the normal
cavities the field Hj
is maximum at the outer surface of the drift tube and not at the cavity radius.
Therefore the frequency sensitivity of the cavity radius is much smaller as
compared to that of the drift tube outer surface. Therefore we could squeeze the
cavity diameter further to make it more compact. Figure 5 shows the geometrical
details of INDUS-1 and booster cavity.
Fig. 5 Geometric
details of INDUS-1 RF cavity
Table-2: Design Parameters of
RF Cavities for synchrotron and storage ring.
Provision for HOM damping
The study of field distributions of the Higher
Order Modes reveals that almost all of them have strong radial electric field
on the cylindrical boundary. Therefore it
was decided to use damping probes or antennae which will couple only to the
radial electric field as the loop couplers are bound to couple to the
fundamental mode which is undesirable. Based on this, there are in all five
ports provided at these points on the cylindrical wall of the cavity for
mounting the damping antennae.
4 RADIO frequency knock-out system
(RFKQ)
system is employed to measure betatron tunes in Booster & Indus-1 ring, In
Booster Synchrotron pairs of open plate electrodes are installed as beam shaker.
These electrodes require RF voltage of 0 -1000 volts at frequency range of 1 to
5 MHz. A wide band 200 watts RF amplifier has been used. The voltage level of
1000 volts is obtained by transmission line type voltage/ impedance
transformers. RFKO unit of Indus-l storage ring uses pairs of striplines
installed as beam shakers electrodes. Each strip line is excited

Fig 6.
RF Knock out System for INDUS-1
with 100 volts RF signal
with frequency variable from 1 to 10 MHz. The other strip line is excited with
same signal with phase difference of 180o. Indus-l RFKO amplifier
system consists of two units of 300 watts wideband RF amplifier modules driven
at 180° phase difference . 300 watts of RF amplifier unit is designed with BEL
make RF power transistor S175-28 operating in class AB push pull mode. Two such
units are driven by 180° power splitter.
5 ION clearing electrode RF system
Circulating electron beam ionizes the residual
gas molecules in the vacuum chamber of Indus-1. These positively charged
particles remain trapped near the design orbit due to the attractive potential
of the electron beam and may give rise to instability. To keep the ion
concentration below a certain value, 8 numbers of Ion clearing electrodes are
installed at various locations in the vacuum chamber. These electrodes are
biased with 1 KV DC superimposed with 200 volts peak to peak RF voltage. The
frequency is sweeped at 1 -4 MHz with sweep rate ranging from 10 mS to 100 mS.
The solid state RF amplifier with output power of 80 watt is built. In phase
power splitter is developed to feed the power to eight ion clearing electrodes.
RF voltage at each port is then boosted to 200 volt by transmission line type
high voltage hybrid transformer and 1 KV DC voltage is superimposed with RF at
these transformers. Low power (2 watts) module is designed with RF transistors
2N 5070 operating in class AB push pull mode and power module is designed with
RF transistors S 50 -28 operating in class AB push pull mode. This RF amplifier
along with SCR controlled 1 KV / 200 mA regulated DC power supply is housed in a
19" rack. Thruline type reflectometer cum VSWR Protection System is used to
monitor forward and reflected powers of RF amplifier and to switch off DC supply
of RF amplifier in case of excessive reflection from the electrodes.

Fig 7. Ion clearing RF
system for INDUS-1
4 MICROWAVE system for injector microtron
Microwave system for the 20 MeV injector-microtron,
developed indigenously, consists of a 5MW S-Band klystron, 130 kV klystron pulse
modulator and a WR-284 wave-guide transmission line. The microwave power to the
microtron accelerating cavity is transmitted by means of the wave-guide line
which consists of four-port circulator, dual directional coupler, wave-guide
pressurizing unit, microwave window and dummy loads. The power from a stabilized
signal generator at 2856 MHz is amplified up to 200 W by means of solid state
amplifier and a solid state modulator driven klystron driver amplifier chain.
The pulse modulator is made of a regulated high voltage 15kV DC supply, a
charging choke, charging diode assembly, pulse forming network, high voltage
thyratron and 1:10 pulse transformer whose bifilar wound secondary is connected
to the device to supply the beam voltage to klystron in pulses of 3.6 sec
duration at 1 Hz repetition rate. A fully automatic dry air pressurization
system has been incorporated to replace the nitrogen cylinder based system. An
all-solid state pulse modulator, giving 4kV, 10 sec
pulses, has been developed to drive the driver klystron of the microwave system.
All the technologies related to the microwave
system like the development of pulse forming networks, pulse transformers,
complete interlock systems, thyratron trigger drives, high voltage capacitive
dividers and pulse current transformers, klystron high voltage deck, driver
amplifier, waveguide sections, dual directional couplers, microwave windows and
high power water loads are developed indigenously. The microwave system has
completed over 10 years (more than 44,000- hours) of continuous and successful
operation.

Fig. 8. 5MW klystron and
compact waveguide line with the Injector Microtron. On the back side is seen the
klystron modulator.
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Table-5
Specifications of the 5MW microwave System |
|
Peak output power |
5 |
MW |
|
Pulse duration |
4 |
sec
|
|
Pulse repetition rate |
1-3 |
Hz |
|
Klystron beam voltage
|
127 |
kV |
|
Klystron beam current |
87 |
A |
|
Rise time |
0.5 |
sec |
|
Fall time |
0.8 |
sec |

Fig. 9 From top
oscilloscope traces of reflected power from cavity, microtron output beam
current 23 mA, microwave forward power detected pulse at 2.6 MW, and electron
emission current from cathode 560mA. Horizontal scale is 500nS/Div.
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